WEBVTT 1 00:00:04.980 --> 00:00:10.920 SLOS TRXI is an x ray imager used on OMEGA. It is a 2 00:00:10.920 --> 00:00:14.820 fixed diagnostic mounted onto the system at Port h four and is 3 00:00:14.820 --> 00:00:19.320 only removed once a year for routine maintenance. Anytime it 4 00:00:19.320 --> 00:00:22.800 is removed or re installed onto the system, experimental 5 00:00:22.800 --> 00:00:25.890 technicians must work cleanroom suits, which helps protect the 6 00:00:25.890 --> 00:00:31.500 entire Omega system from dust and debris. TRXI is capable of 7 00:00:31.500 --> 00:00:35.730 taking multiple frames with a 40 picosecond temporal resolution 8 00:00:35.820 --> 00:00:40.680 at a 10 micron spatial resolution. This is achieved by 9 00:00:40.680 --> 00:00:43.680 combining an electron pulse dilation imager with a fast 10 00:00:43.680 --> 00:00:50.190 gated sensor. It captures X rays in a four to nine KV range 11 00:00:50.220 --> 00:00:55.110 around the time of peak compression during ICF. SLOS 12 00:00:55.110 --> 00:00:58.260 TRXI is used to determine the size of the core of imploded 13 00:00:58.260 --> 00:01:02.550 cryogenic targets at stagnation. This allows for the inference of 14 00:01:02.550 --> 00:01:03.690 the hotspot pressure. 15 00:01:05.550 --> 00:01:10.950 The imager on SLOS TRXI is a pinhole array, about 30 images 16 00:01:10.950 --> 00:01:14.700 of the hotspot can be obtained per frame, and these individual 17 00:01:14.700 --> 00:01:18.120 pinhole images are average to increase the signal to noise 18 00:01:18.120 --> 00:01:18.780 ratio. 19 00:01:21.780 --> 00:01:24.930 The photons are then incident on the photocathode and produce 20 00:01:24.930 --> 00:01:30.060 electrons via the photoelectric effect. The photocathode is a 21 00:01:30.060 --> 00:01:33.840 transmission photocathode where photons are incident on one side 22 00:01:33.870 --> 00:01:35.730 and electrons lead from the other side. 23 00:01:38.700 --> 00:01:42.690 To colliding high voltage pulses travel across the photocathode 24 00:01:42.960 --> 00:01:47.580 and some to create a spatially uniform voltage profile. The 25 00:01:47.580 --> 00:01:51.330 photocathode voltage varies in time, and the kinetic energies 26 00:01:51.360 --> 00:01:56.130 of the electrons are time dependent. So electrons that are 27 00:01:56.130 --> 00:01:59.670 born earlier in time have a higher velocity than electrons 28 00:01:59.670 --> 00:02:00.750 born later in time. 29 00:02:04.080 --> 00:02:07.410 The electron cloud then enters the drift region which is held 30 00:02:07.410 --> 00:02:13.620 at a constant potential. The electron cloud elongates as it 31 00:02:13.620 --> 00:02:16.800 travels down the drift tube due to the differing velocities. 32 00:02:18.990 --> 00:02:21.930 There is a solenoid around the drift tube to produce an axial 33 00:02:21.930 --> 00:02:25.050 magnetic field that prevents the transverse spread of the 34 00:02:25.050 --> 00:02:30.990 electron cloud. Due to the high voltages in the imaging system, 35 00:02:31.080 --> 00:02:34.410 the drift tube is held at a high vacuum to prevent electrical 36 00:02:34.410 --> 00:02:34.950 arcing. 37 00:02:37.800 --> 00:02:41.400 The electrons are detected on multiple frames of an HC MOS 38 00:02:41.400 --> 00:02:45.300 sensor, which is a 2d detector developed at Sandia National 39 00:02:45.300 --> 00:02:52.380 Laboratories. The detector is time resolved, with about a 2.5 40 00:02:52.380 --> 00:02:56.910 nanosecond gate time per frame. Coupled with the drift tube, 41 00:02:57.240 --> 00:03:00.540 which has a temporal magnification of about 80 times 42 00:03:00.870 --> 00:03:04.740 the effective gate time is approximately 35 to 40 pico 43 00:03:04.740 --> 00:03:05.370 seconds. 44 00:03:08.400 --> 00:03:12.750 Here's an unprocessed readout of the H CMOS sensor. You can see 45 00:03:12.750 --> 00:03:16.080 the images are changing in time getting brighter from frame one 46 00:03:16.080 --> 00:03:20.400 to frame to. The individual pinhole images are then cut out 47 00:03:20.820 --> 00:03:26.550 and added together to create a composite image. On the right is 48 00:03:26.550 --> 00:03:32.400 how the image compares one to 510 and 29 separate images are 49 00:03:32.400 --> 00:03:33.540 included in the stack 50 00:03:35.970 --> 00:03:39.360 SLOS TRXI is the second time resolved X ray imager used on 51 00:03:39.360 --> 00:03:44.160 OMEGA a third time resolved X ray imager is currently being 52 00:03:44.160 --> 00:03:49.080 designed and will operate similarly to SLOS TRXI. This 53 00:03:49.080 --> 00:03:52.020 third line of sight will have approximately a 20 picosecond 54 00:03:52.020 --> 00:03:55.530 temporal resolution and a five micron spatial resolution. 55 00:03:57.270 --> 00:04:00.900 The three time resolved X ray images will be used together to 56 00:04:00.900 --> 00:04:04.170 help us understand how the hotspot evolves in time, the 57 00:04:04.170 --> 00:04:07.680 multi dimensional effects that occurred during ICF implosions 58 00:04:08.100 --> 00:04:11.160 and to create a 3D reconstruction of the hotspot